Fig. 12.
Left: Schematic view of the filament formation process due to compression of an overdensity by a shock wave (adapted from Inoue et al. 2018). The ambient B-field (indicated by the black lines) is parallel to the shock front. Right: Blow-up of the PV diagram (see figure 8) in 13CO(1–0) towards the filament YF for velocities between 6.8 km s−1 and 9 km s−1. The filament and the parent extended sheet-like structure are indicated with a white circle and a gray ellipse, respectively. The velocity gradients induced by the bending of the magnetic field are shown as converging arrows towards the filament (cf. subsection 4.2). (Color online)

Left: Schematic view of the filament formation process due to compression of an overdensity by a shock wave (adapted from Inoue et al. 2018). The ambient B-field (indicated by the black lines) is parallel to the shock front. Right: Blow-up of the PV diagram (see figure 8) in 13CO(1–0) towards the filament YF for velocities between 6.8 km s−1 and 9 km s−1. The filament and the parent extended sheet-like structure are indicated with a white circle and a gray ellipse, respectively. The velocity gradients induced by the bending of the magnetic field are shown as converging arrows towards the filament (cf. subsection 4.2). (Color online)

Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close